2015/11/30 by D. E. Kharzeev, Dmitri E. Kharzeev, J. Liao +3 · 29 citations
Physics and Astronomy · #Dissipative system #Gauge theory #Gluon #High-Energy Particle Collisions Research #Magnetic field #Nuclear physics #Particle physics #Physics #Plasma #Pulsars and Gravitational Waves Research #Quantum Chromodynamics and Particle Interactions #Quantum chromodynamics #Quantum electrodynamics #Quantum mechanics #Quark #Quark–gluon plasma #cond-mat.str-el #hep-ph #hep-th #nucl-ex #nucl-th
paper · pdf · doi:10.1016/j.ppnp.2016.01.001
Invited review for Progress in Particle and Nuclear Physics; 38 pages, 25 figures; v2 matching published version
openalex publication_date 2016/01/16 · arxiv created 2016/03/19 · arxiv updated 2016/03/23 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
The interplay of quantum anomalies with magnetic field and vorticity results in a variety of novel non-dissipative transport phenomena in systems with chiral fermions, including the quark-gluon plasma. Among them is the Chiral Magnetic Effect (CME) -- the generation of electric current along an external magnetic field induced by chirality imbalance. Because the chirality imbalance is related to the global topology of gauge fields, the CME current is topologically protected and hence non-dissipative even in the presence of strong interactions. As a result, the CME and related quantum phenomena affect the hydrodynamical and transport behavior of strongly coupled quark-gluon plasma, and can be studied in relativistic heavy ion collisions where strong magnetic fields are created by the colliding ions. Evidence for the CME and related phenomena has been reported by the STAR Collaboration at Relativistic Heavy Ion Collider at BNL, and by the ALICE Collaboration at the Large Hadron Collider at CERN. The goal of the present review is to provide an elementary introduction into the physics of anomalous chiral effects, to describe the current status of experimental studies in heavy ion physics, and to outline the future work, both in experiment and theory, needed to eliminate the existing uncertainties in the interpretation of the data.